Yunna Tushinova , Sesegma Dorzhieva , Aleksandra Logvinova , Bair Bazarov , Aleksandr Aleksandrovsky , Alexander Krylov , Nikolai Maximov , Maxim Molokeev , Aleksandr Oreshonkov , Victor Atuchin
{"title":"Negative thermal expansion effects, spectroscopic properties and electronic structure transformations in Tm2Zr(MoO4)5","authors":"Yunna Tushinova , Sesegma Dorzhieva , Aleksandra Logvinova , Bair Bazarov , Aleksandr Aleksandrovsky , Alexander Krylov , Nikolai Maximov , Maxim Molokeev , Aleksandr Oreshonkov , Victor Atuchin","doi":"10.1016/j.materresbull.2025.113485","DOIUrl":null,"url":null,"abstract":"<div><div>New noncentrosymmetric molybdate Tm<sub>2</sub>Zr(MoO<sub>4</sub>)<sub>5</sub> was synthesized. The crystal structure variation with temperature was determined by Rietveld analysis. At 303 K, the monoclinic structure was determined in space group <em>P</em>2<sub>1</sub>. A reversible phase transition <em>P</em>2<sub>1</sub>↔<em>Cmc</em>2<sub>1</sub> was found at 390 K. From 423 to 520 K, nearly a ZTE (α = 0.7 × 10<sup>−6</sup> K<sup>−1</sup>) behavior was revealed. In the range of 520–720 K, the negative thermal expansion (NTE) effect (α = -2.3 × 10<sup>−6</sup> K<sup>−1</sup>) is evident for the cell volume. Tm<sub>2</sub>Zr(MoO<sub>4</sub>)<sub>5</sub> is stable up to 1100 K. Electronic structures of monoclinic and orthorhombic Tm<sub>2</sub>Zr(MoO<sub>4</sub>)<sub>5</sub> were evaluated by DFT methods. The bandgap values determined for monoclinic Tm<sub>2</sub>Zr(MoO<sub>4</sub>)<sub>5</sub> are E<sub>g direct</sub> = 3.83 eV and E<sub>g indirect</sub> = 3.43 eV. The vibrational properties of monoclinic phase were characterized by Raman spectroscopy. The photoluminescence emission in monoclinic Tm<sub>2</sub>Zr(MoO<sub>4</sub>)<sub>5</sub> at 303 K is dominated by a narrower band at 650 nm due to the <sup>1</sup>G<sub>4</sub> - <sup>3</sup>F<sub>4</sub> transition.</div></div>","PeriodicalId":18265,"journal":{"name":"Materials Research Bulletin","volume":"190 ","pages":"Article 113485"},"PeriodicalIF":5.3000,"publicationDate":"2025-04-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Materials Research Bulletin","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S002554082500193X","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
New noncentrosymmetric molybdate Tm2Zr(MoO4)5 was synthesized. The crystal structure variation with temperature was determined by Rietveld analysis. At 303 K, the monoclinic structure was determined in space group P21. A reversible phase transition P21↔Cmc21 was found at 390 K. From 423 to 520 K, nearly a ZTE (α = 0.7 × 10−6 K−1) behavior was revealed. In the range of 520–720 K, the negative thermal expansion (NTE) effect (α = -2.3 × 10−6 K−1) is evident for the cell volume. Tm2Zr(MoO4)5 is stable up to 1100 K. Electronic structures of monoclinic and orthorhombic Tm2Zr(MoO4)5 were evaluated by DFT methods. The bandgap values determined for monoclinic Tm2Zr(MoO4)5 are Eg direct = 3.83 eV and Eg indirect = 3.43 eV. The vibrational properties of monoclinic phase were characterized by Raman spectroscopy. The photoluminescence emission in monoclinic Tm2Zr(MoO4)5 at 303 K is dominated by a narrower band at 650 nm due to the 1G4 - 3F4 transition.
期刊介绍:
Materials Research Bulletin is an international journal reporting high-impact research on processing-structure-property relationships in functional materials and nanomaterials with interesting electronic, magnetic, optical, thermal, mechanical or catalytic properties. Papers purely on thermodynamics or theoretical calculations (e.g., density functional theory) do not fall within the scope of the journal unless they also demonstrate a clear link to physical properties. Topics covered include functional materials (e.g., dielectrics, pyroelectrics, piezoelectrics, ferroelectrics, relaxors, thermoelectrics, etc.); electrochemistry and solid-state ionics (e.g., photovoltaics, batteries, sensors, and fuel cells); nanomaterials, graphene, and nanocomposites; luminescence and photocatalysis; crystal-structure and defect-structure analysis; novel electronics; non-crystalline solids; flexible electronics; protein-material interactions; and polymeric ion-exchange membranes.